相位调制信号对窄线宽光纤放大器线宽特性和受激布里渊散射阈值的影响

高功率窄线宽光纤放大器的输出功率主要受限于受激布里渊散射(SBS)效应,通过相位调制进行线宽展宽可以有效抑制SBS效应.基于窄线宽光纤放大器中的SBS动力学模型,研究了正弦信号、白噪声信号和伪随机编码信号(PRBS)对窄线宽光纤放大器光谱特性与SBS阈值的影响.研究发现,采用不同信号进行相位调制时,调制频率和调制深度等参数对调制后激光光谱的谱线间隔、谱线数目与光谱平整度的影响存在较大差异,进而影响放大器的线宽特性和SBS阈值.通过对比分析,给出了调制信号的类型选择和参数优化原则,能够为窄线宽光纤放大器的相位调制系统设计提供参考.     

窄线宽纳秒脉冲光纤拉曼放大器的理论模型和数值分析

窄线宽纳秒脉冲光纤拉曼放大器在非线性频率变换、遥感探测和量子信息等领域有广泛的应用前景.综合考虑受激拉曼散射(stimulated Raman scattering,SRS)、受激布里渊散射(stimulated Brillouin scattering,SBS)、自相位调制(self-phase modulation)和交叉相位调制(cross-phase modulation)等非线性效应,建立了窄线宽纳秒脉冲光纤拉曼放大器的非线性动力学模型.仿真分析了放大器中脉冲激光的时频演化特性,对比研究了抽运脉冲宽度、光纤长度和信号光功率等因素对放大器性能的影响.研究发现,上述因素会影响放大器的SRS阈值、SBS阈值、输出激光线宽、激光转换效率等.例如,当脉冲宽度为800 ns时,SBS随着抽运功率的增加而发生,限制了激光功率的提升;减短抽运脉宽可以抑制SBS,但是输出激光的线宽易于展宽到数百MHz以上;增加光纤长度可以获得更低的SRS阈值和更高的转换效率,但是SBS效应和光谱展宽程度也随之增强.系统搭建中需要平衡各非线性效应,选择合适的系统参数.研究内容可以为窄线宽纳秒脉冲光纤拉曼放大器的设计搭建提供参考.     

780W全光纤窄线宽光纤激光器

高功率窄线宽光纤激光器在相干探测、功率光谱合成等方面具有广泛的应用前景.分析了高功率窄线宽光纤激光器中受激布里渊散射效应的抑制方法,以及正弦相位调制光谱展宽理论.采用正弦相位调制技术将单频激光器的线宽展宽至2.9 GHz,通过三级放大结构对输出功率为50 mW的窄线宽种子源进行放大,实现了中心波长1064.34 nm、线宽2.9 GHz、最大功率780 W的激光输出,光—光转换效率79%,光束质量M2x=1.44,M2y=1.43.分析了相位调制前后输出功率提高的原因,认为正弦相位调制增加的纵模降低了光纤中的功率谱密度,提高了输出激光的受激布里渊散射阈值,促使相位调制后的输出功率大幅提高.该激光器的输出功率仅受限于抽运功率,进一步提高抽运功率,有望实现更高功率的窄线宽光纤激光输出.     

百皮秒脉冲放大中自相位调制效应实验研究

利用掺镱双包层光纤放大器对百皮秒单脉冲（重复频率1 Hz）进行了放大实验,分析了其放大过程中自相位调制对脉冲时域和频域特性的影响.采用小芯径（纤芯直径6.5 μm）掺镱双包层光纤作为增益介质,研究了放大器中从小信号增益到增益深度饱和整个变化过程中自相位调制引起的频谱展宽效应,并分析了SPM引起的脉冲波形和频谱光强分布的变化.采用布喇格光纤光栅扫描方法观察了其光谱的变化,解决了单脉冲光谱不易测量的问题.结果表明：区别于无源光纤中的自相位调制效应,随着抽运功率的增加,百皮秒脉冲放大过程中增益饱和效应和自相位调制效应的共同作用,使脉冲频谱分裂成不对称双峰结构,且光强分布先向短波后逐渐向长波集中.     

基于多光子脉冲内干涉相位扫描法对飞秒激光脉冲进行相位测量和补偿的研究

研制了一套基于多光子脉冲内干涉相位扫描方法的可以同时对飞秒激光脉冲进行相位测量和补偿的实验系统装置.实验中,通过自主研发的LabVIEW程序控制液晶空间光调制器和光纤光谱仪,对待测飞秒激光脉冲施加相位扫描,并同时记录受到调制的飞秒激光脉冲的倍频光谱,得到了多光子脉冲内干涉相位扫描(MIIPS)轨迹图.通过MIIPS轨迹图的三次测量和迭代运算,还原出了经过预先啁啾调制的中心波长约为810 nm、重复频率为1 kHz的飞秒激光脉冲的光谱相位,测量精度在0.1 rad以内.根据测量结果,利用液晶空间光调制器对该飞秒激光脉冲进行相位补偿,得到了近似傅里叶变换极限的飞秒激光脉冲.这一装置将在多光子显微成像、脉冲整形、飞秒激光光谱学等众多领域发挥重要作用.     

1.06kW 13GHz线宽全光纤激光器

分析了高功率光纤激光器中受激布里渊散射(SBS)效应的抑制方法。研究表明,利用宽带噪声源高速相位调制展宽光谱的方法对于抑制SBS十分有效,可实现kW级用于光谱组束的数10GHz高功率光纤激光子束。通过理论计算线宽与SBS阈值的关系,并分析噪声相位调制各参数对SBS阈值提升的影响,优化了光纤激光器设计参数。通过宽带噪声高速相位调制的方法,展宽单频种子源线宽至13GHz,通过两级预放大至10 W后,使用20/400μm掺Yb光纤最终实现了中心波长1064nm、线宽13GHz、最高功率1.06kW的激光输出,光束质量M21.2,光-光转换效率86%,实验过程未观测到模式不稳定性现象。进一步扩宽噪声源频带,加大调制深度,有望实现更高功率的窄线宽光纤激光输出。     

啁啾光脉冲的振幅调制和相位扰动对压缩光脉冲的影响

 通过采用分步傅里叶变换法求解非线性薛定谔方程，模拟了啁啾光脉冲有振幅调制和相位扰动下的自相位调制（SPM）对压缩光脉冲对比度和预脉冲宽度的影响。结果表明：啁啾光脉冲的振幅调制深度和相位扰动深度越大，则压缩后的光脉冲对比度越小；啁啾光脉冲的振幅调制周期和相位扰动周期越小，则压缩光脉冲的预脉冲宽度越大。     

半导体激光放大器用于啁啾补偿的研究

详细分析了饱和工作状态下的行波半导体激光放大器的啁啾特性，从理论上证了实了利用其增益饱和所引起的自相位调制来对光源啁啾和光纤色散进行啁啾补偿的可行性，并且发现，对于不同脉宽的入射脉冲，光放大器均能发挥相位补偿的作用，这一特性可用来在长距离光纤传输系统中，对微弱啁光脉冲同时进行能量和相位的补偿。     

亚百飞秒高功率掺镱大模面积光子晶体光纤飞秒激光放大器的实验研究

实验研究了掺镱双包层保偏大模面积光子晶体光纤飞秒激光放大器. 获得了平均功率达16W的飞秒激光放大输出,在50MHz重复频率下,对应的单脉冲能量达到320nJ. 增益光纤长3.5m,由于自相位调制效应,种子光脉冲光谱在放大过程中同时展宽,从而支持更窄的脉冲宽度. 经过光栅后,脉冲宽度压缩到了85fs. 系统中的振荡器和放大器基于同一种具有偏振结构的大模面积光子晶体光纤,具有很好的环境稳定性和进一步集成的可能. 关键词： 光子晶体光纤 大模场面积光纤 飞秒激光 光纤放大器     

基于时间透镜系统的冲击脉冲产生与特性研究

冲击点火方案具备低点火能量阈值、高增益以及更好的流体力学稳定性等优势,已成为实现惯性约束聚变点火的核心方案之一.在冲击点火方案中,高质量的冲击脉冲是实现成功点火的必要条件.本文基于光纤环相位调制时间透镜系统,提出一种利用时域非对称相位调制结合频域线性色散补偿的方案产生对脉宽和峰值功率对比度高精度可控的冲击脉冲,并构建了理论模型,通过数值模拟详细分析了系统关键参数对冲击脉冲特性的影响.模拟结果显示,通过对斩波函数、相位调制函数、调制深度、调制频率以及啁啾补偿量等参数的组合优化设计,可以实现对冲击脉冲的脉冲宽度、脉冲上升沿以及冲击脉冲峰值功率对比度等关键性能指标高精度主动调控.这种对冲击脉冲峰值功率对比度与冲击脉冲宽度独立主动可调的新型设计思路,不仅有利于加深对激光脉冲波形操控原理的理解,而且对实验上如何获取高质量的冲击脉冲具有重要参考意义.     

Mean displacement moments and survival times in the trapping model with strong fields

The mean displacement moments for the strong field trapping model are calculated. Their asymptotic behaviour is Xⁿ(t) (V_efft)ⁿ, where V_eff is an effective drift velocity. This is in sharp contrast with the weak field case, for which Xⁿ(t) t^n/3. The mean survival (first passage) time and the upstream and downstream trapping probabilities are also obtained.     

Ge-Sb-Se硫系玻璃的折射率和热光系数

Ge-Sb-Se硫系玻璃被认为是极佳的红外传输材料和有潜力的非线性光学材料.在光学设计中,玻璃的线性折射率(n)及其热光系数(ζ)是关键技术参数.以预测和调控Ge-Sb-Se玻璃的n和ζ为目的,考察了玻璃的n,ζ,密度(d)和体积膨胀系数(β)与化学参数dSe和拓扑网络结构参数r的内在联系.研究发现,玻璃的n随d的增加而增大;ζ随β的增大而近似线性减小;β随dSe的减小或r的增大而减小;当Ge含量固定时, d随dSe的减小或r的增大而增大,当Sb含量固定时, d在dSe=0时具有最小值.基于实测d和n,拟合获得了Ge, Sb和Se元素在2—12μm波段的摩尔折射度(R_i),分别为R_(Ge)=10.16—10.50 cm~3/mol,RSb=16.71—17.08 cm~3/mol和RSe=11.15—11.21 cm~3/mol,根据d和R_i计算得到的n与实测值的偏差小于1%.基于实测ζ和β,拟合得到了Ge, Sb和Se元素在2—12μm波段的摩尔折射度温度系数(φ_i),分别为φ_(Ge)=21.1—22.6 ppm/K,φ_(Sb)=7.2—8.4 ppm/K和φ_(Se)=90.2—94.2 ppm/K,根据β和φ_i计算得到的ζ与实测值的偏差小于6 ppm/K.     

Magnetic dynamics of two-dimensional itinerant ferromagnet Fe_3GeTe_2

Among the layered two-dimensional ferromagnetic materials(2 D FMs),due to a relatively high T_C,the van der Waals(vdW) Fe_3 GeTe_2(FGT) crystal is of great importance for investigating its distinct magnetic properties.Here,we have carried out static and dynamic magnetization measurements of the FGT crystal with a Curie temperature TC ≈ 204 K.The M-H hysteresis loops with in-plane and out-of-plane orientations show that FGT has a strong perpendicular magnetic anisotropy with the easy axis along its c-axis.Moreover,we have calculated the uniaxial magnetic anisotropy constant(K_1)from the SQUID measurements.The dynamic magnetic properties of FGT have been probed by utilizing the high sensitivity electron-spin-resonance(ESR) spectrometer at cryogenic temperatures.Based on an approximation of single magnetic domain mode,the K_1 and the effective damping constant(α_(eff)) have also been determined from the out-of-plane angular dependence of ferromagnetic resonance(FMR) spectra obtained at the temperature range of 185 K to T_C.We have found large magnetic damping with the effective damping constant α_(eff) ～ 0.58 along with a broad linewidth(ΔH_(pp) 1000 Oe at 9.48 GHz,H ‖ c-axis).Our results provide useful dynamics information for the development of FGT-based spintronic devices.     

Ferromagnetic resonance in Sr doped rare earth orthocobaltites, Ln1−xSrxCoO3†

FMR measurements have been carried out on several members of the Ln_1−xSrxCoO₃ (Ln = Rare earth) system. The results show that g_eff in these systems is around 1.25 independent of x as well as the rare earth ion. It is suggested that this unusual value of g_eff is due to the localized intermediate-spin Co³⁺ ions (t⁵_2g e¹_g) located at the top of the π^* band.     

Effects of short-range attraction on Jamming transition

Enormous progresses to understand the jamming transition have been driven via simulating purely repulsive particles which were somehow idealized in the past two decades. While the attractive systems are both theoretical and practical compared with repulsive systems. By studying the statistics of rigid clusters, we find that the critical packing fraction φ_c varies linearly with attraction μ for different system sizes when the range of attraction is short. While for systems with long-range attractions, however, the slope of φ_c appears significantly different, which means that there are two distinct jamming scenarios. In this paper, we focus our main attention on short-range attractions scenario and define a new quantity named "short-range attraction susceptibility" χ_p, which describes the degree of response of the probability of finding jammed states pjto short-range attraction strength μ. Our central results are that χ_p diverges in the thermodynamic limit as χ_p ∝|φ-φ_c~∞|~(-γ_p), where φ_c~∞ is the packing fraction at the jamming transition for the infinite system in the absence of attraction. χ_p obeys scaling collapse with a scaling function in both two and three dimensions, illuminating that the jamming transition can be considered as a phase transition as proposed in previous work.     

Effects of collision energy and rotational quantum number on stereodynamics of the reactions:H(~2S)+NH(v=0,j=0,2,5,10)→N(~4S)+H_2

The stereodynamical properties of H(~2S) + NH(v = 0,j = 0,2,5,10)→N(~4S) + H_2 reactions are studied in this paper by using the quasi-classical trajectory(QCT) method with different collision energies on the double many-body expansion(DMBE) potential energy surface(PES)(Poveda L A and Varandas A J C 2005 Phys.Chem.Chem.Phys.7 2867).In a range of collision energy from 2 to 20 kcal/mol,the vibrational rotational quantum numbers of the NH molecules are specifically investigated on v = 0 and j = 0,2,5,10 respectively.The distributions of P(θ_r),P(φ_r),P(θ_r,φ_r),(2π/σ)(dσ_(00)/dω_t)differential cross-section(DCSs) and integral cross-sections(ICSs) are calculated.The ICSs,computed for collision energies from 2 kcal/mol to 20 kcal/mol,for the ground state are in good agreement with the cited data.The results show that the reagent rotational quantum number and initial collision energy both have a significant effect on the distributions of the k-j',the k-k'-j',and the k-k' correlations.In addition,the DCS is found to be susceptible to collision energy,but it is not significantly affected by the rotational excitation of reagent.     

He原子体系中偶极子响应的周期性量子相位调控的理论研究

基于激光诱导相位模型, 研究了周期性相位调控的He原子体系的光谱响应. 研究发现,周期性的相位调控会导致He原子吸收谱由单个孤立的洛伦兹线型转化为等间隔的“梳状”结构. “梳状”光谱的性质主要由原子系统和控制脉冲链的性质决定, 并给出了表征“梳状”光谱的理论公式. 该机理具有普遍适用性, 它可以应用到任意原子体系, 进而推广到任意波段, 并且为任意波段的脉冲整形提供了可能.